Tapader Dhiraj, Pradhan Punyabrata, Dhar Deepak
Department of Theoretical Sciences, S. N. Bose National Centre for Basic Sciences, Block-JD, Sector-III, Salt Lake, Kolkata 700106, India.
Department of Physics, Indian Institute of Science Education and Research, Pune, Dr. Homi Bhabha Road, Pashan, Pune 411008, India.
Phys Rev E. 2021 Mar;103(3-1):032122. doi: 10.1103/PhysRevE.103.032122.
We study relaxation of long-wavelength density perturbations in a one-dimensional conserved Manna sandpile. Far from criticality where correlation length ξ is finite, relaxation of density profiles having wave numbers k→0 is diffusive, with relaxation time τ_{R}∼k^{-2}/D with D being the density-dependent bulk-diffusion coefficient. Near criticality with kξ≳1, the bulk diffusivity diverges and the transport becomes anomalous; accordingly, the relaxation time varies as τ_{R}∼k^{-z}, with the dynamical exponent z=2-(1-β)/ν_{⊥}<2, where β is the critical order-parameter exponent and ν_{⊥} is the critical correlation-length exponent. Relaxation of initially localized density profiles on an infinite critical background exhibits a self-similar structure. In this case, the asymptotic scaling form of the time-dependent density profile is analytically calculated: we find that, at long times t, the width σ of the density perturbation grows anomalously, σ∼t^{w}, with the growth exponent ω=1/(1+β)>1/2. In all cases, theoretical predictions are in reasonably good agreement with simulations.
我们研究了一维守恒曼纳沙堆中长波长密度扰动的弛豫。在远离临界状态(此时关联长度ξ是有限的)时,波数k→0的密度分布的弛豫是扩散性的,弛豫时间τ_{R}∼k^{-2}/D,其中D是与密度相关的体扩散系数。在kξ≳1的临界状态附近,体扩散率发散,输运变得反常;相应地弛豫时间随τ_{R}∼k^{-z}变化,动力学指数z = 2 - (1 - β)/ν_{⊥}<2,其中β是临界序参量指数,ν_{⊥}是临界关联长度指数。在无限临界背景上初始局域化密度分布的弛豫呈现出自相似结构。在这种情况下,解析计算了随时间变化的密度分布的渐近标度形式:我们发现长时间t时,密度扰动的宽度σ反常增长,σ∼t^{w},增长指数ω = 1/(1 + β)>1/2。在所有情况下,理论预测与模拟结果相当吻合。